一维势垒散射中粒子的概率分布

利用数值计算方法研究了E>U0、0相似文献   

基于后验概率度量的粒子滤波跟踪算法研究

 针对遮挡、光照变化、尺度变化等复杂环境中的视觉跟踪问题,提出一种基于后验概率度量的粒子滤波跟踪算法。由于后验概率指标与Bhattacharyya系数指标相比具有更强的峰值特性,采用后验概率指标作为相似性度量函数,通过粒子的更新、推广、观测、估计等步骤实现跟踪算法。通过对实际视频图像序列进行目标跟踪实验,实验结果表明:传统算法只有约50%的图像能够实现尺度自适应,而本文算法采用传统算法25%的粒子就能够收敛逼近目标的真实轨迹,达到更强的抗遮挡能力,90%以上的图像序列都能够实现良好的尺度自适应效果。     

线度和势垒宽度对球状纳米系统电子散射截面的影响

在有效质量近似和球形方形势模型下,计算了开放型球状纳米系统电子散射截面及电子按能量的概率分布,探讨了线度、势垒宽度对电子散射截面和共振能量以及共振宽度的影响.结果表明:电子的散射截面随能量的分布曲线有一极大值和极小值,而且电子能量的概率分布曲线的极大值位置总是介于散射截面分布曲线的极大值与极小值的能量位置之间;散射截面随内核半径r₀的增大而增大,而且散射截面分布曲线随r₀的增大由较平滑变得较尖锐;散射截面随势垒宽度Δ的增大而增大,但在Δ＝1.4a_CdS–1.7a_CdS的范围内,变化出现异常,在Δ=1.6a_CdS时散射截面出现极小;电子共振能量E_l 随Δ的变化与电子所处状态有关,而电子共振宽度Γ_l随Δ的增大而减小;不论Δ取何值, E_l和Γ_l都满足能量和时间的测不准关系. 关键词： 球状纳米系统 势垒宽度 电子散射截面 电子概率分布     

How likely is Polya's drunkard to stay in x⩾ y⩾z?

In his celebrated paper, Polya has considered the random walk in the three-dimensional (cubic) lattice and showed that the probability of return to the origin is less than 1. Subsequent authors have shown that the probability is %34.053.... Here we consider the same random walk, with the restriction that the drunkard is only allowed to stay inxyz. It is shown that his probability of returning to the originand staying in the allowed region is %6.4844....     

90Mo电磁跃迁几率的测量

利用束流能量为116MeV的⁵⁹Co(³⁵Cl,2p2n)⁹⁰Mo反应布居⁹⁰Mo的高自旋态.用10台反康普顿HPGe探测器组成的探测阵列进行γγ符合测量.通过多普勒展宽峰的形状分析测定⁹⁰Mo高自旋态的寿命.在正宇称衰变系观察到增强的M1跃迁,推断I=13以上是扁椭形变.负宇称高自旋态具有大的B(E2)值,并随自旋增大而起伏变化.正、负宇称态之间的跃迁显示增大的E1跃迁,似有八极关联的可能.但是,⁹⁰Mo并不处在理论预言的存在八极形变的核区内.     

Free probability and the von Neumann algebrasof free groups

This short note summarizes the circumstances of the birth of free probability theory andsome of the recent achievements.     

Lifetime of resonant state in a spherical quantum dot

This paper calculates the lifetime of resonant state and transmission probability of a single electron tunnelling in a spherical quantum dot (SQD) structure by using the transfer matrix technique. In the SQD, the electron is confined both transversally and longitudinally, the motion in the transverse and longitudinal directions is separated by using the adiabatic approximation theory. Meanwhile, the energy levels of the former are considered as the effective confining potential. The numerical calculations are carried out for the SQD consisting of GaAs/InAs material. The obtained results show that the bigger radius of the quantum dot not only leads significantly to the shifts of resonant peaks toward the low-energy region, but also causes the lengthening of the lifetime of resonant state. The lifetime of resonant state can be calculated from the uncertainty principle between the energy half width and lifetime.     

低能C36团簇在金刚石(100)晶面沉积时的影响因素

"使用Brenner-LJ拟合势描述了金刚石与C36团簇原子间的相互作用,并用分子动力学模拟的方法研究单个C36(D6h)在金刚石(100)晶面的沉积机制．通过仿真实验分析了C36团簇的入射能量、入射点位置、入射姿势、入射角度等因素对其成核初期化学吸附过程以及沉积后其稳定性的影响．研究发现：由于C36入射点位置及入射姿势的不同,其在金刚石(100)晶面沉积时的沉积阈值最小值为20 eV,最大值为60 eV;在入射角不超过60o斜射时,由于水平运动分量的存在,C36可能翻滚及平滑至成键能量较小的区域后再成键     

PdⅩⅣ-CdⅩⅥ离子4s24p3和4s4p4组态精细结构能级与跃迁的扩展分析

用多组态HXR理论方法对KrⅣ-CdⅩⅥ离子4s^24p^3和4s4p^4组态的精细结构能级进行了分析计算。在已有研究工作的基础上,通过对4s^24p^3和4s4p^4组态能级的实验观测值与HXR计算结果之差AE沿等电子序列变化规律的分析．找出了△E随有效核电荷数Zc变化的规律,预言并计算了PdⅩⅣ-CdⅩⅥ离子4s^24p^3和4s4p^4组态能级,大部分预言计算值与实验结果的偏差小于100cm^-2。由此还进一步计算了PdⅩⅣ-CdⅩⅥ离子4s^24p^3—4s4p^4跃迁的谱线波长、振子强度和跃迁概率。结果表明：除了4s^24p^3D5/2-4s4p^4^2D5/2跃迁的谱线波长(29．992nm)与实验值相差0．018nm外．对于其余5条谱线．预言值与实验值的偏差均不超过0．005nm。     

Study of Survival Probability of Super Heavy Nuclei

The survival probability of super heavy nuclei produced in cold fusion reactions is studied by using the standard Fermi gas level density formula and analyzed with fission and neutron evaporation characteristics predicted in different theoretical models. The level density formula used in this letter suppresses the ratio of neutron emission width to fission width, Гn/Гf. The dependence of Гn/Гf on the saddle point level density parameter and excitation energy is also investigated.